Gravitational Potential Energy
In the position of a particle changes on account of conservative force acting on it, then the changes in its potential energy is just the amount of work done on the body by the conservative forces.
If
is the gravitational force acting on a test mass of mass mo at distance r from the centre of earth, then

Work done in lifting the test mass through displacement
by the internal agent

Total work done in lifting the test mass from r1 to r2 (> r1)

Total work done by gravitational field

= Change in potential energy
If the gravitational potential energy at infinity U1 = 0 and r1 =
and r2 = r, then

Gravitational Potential
Gravitational potential due to gravitational force of the earth is defined as the potential energy of a particle of unit mass at that point.
Potential at position
Relation Between Potential and Field
We have

In vector form
Gravitational Potential Due to Hollow Spherical Shell of Mass M, Radius R
In the position of a particle changes on account of conservative force acting on it, then the changes in its potential energy is just the amount of work done on the body by the conservative forces.
If
Work done in lifting the test mass through displacement
Total work done in lifting the test mass from r1 to r2 (> r1)
Total work done by gravitational field
= Change in potential energy
If the gravitational potential energy at infinity U1 = 0 and r1 =
Gravitational Potential
Gravitational potential due to gravitational force of the earth is defined as the potential energy of a particle of unit mass at that point.
Relation Between Potential and Field
We have
In vector form
Gravitational Potential Due to Hollow Spherical Shell of Mass M, Radius R
- Outside Point (r > R)
- On the surface (r = R)
- Inside the shell (r < R)
Gravitational Potential Due to Solid Sphere of Mass M, Radius R
- Outside point (r > R)
- On the surface (r = R)
- Inside the sphere (r < R)
Gravitational Field for Uniform Solid Sphere of Mass M, Radius R
- Outside point (r > R)
- On the surface (r = R)
- Inside point (r < R)
Variation of (l) with distance (r) from centre

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